WO2018184324A1 - Light source system and projection device - Google Patents
Light source system and projection device Download PDFInfo
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- WO2018184324A1 WO2018184324A1 PCT/CN2017/094797 CN2017094797W WO2018184324A1 WO 2018184324 A1 WO2018184324 A1 WO 2018184324A1 CN 2017094797 W CN2017094797 W CN 2017094797W WO 2018184324 A1 WO2018184324 A1 WO 2018184324A1
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- light
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B21/00—Projectors or projection-type viewers; Accessories therefor
- G03B21/14—Details
- G03B21/20—Lamp housings
- G03B21/208—Homogenising, shaping of the illumination light
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/09—Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/09—Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
- G02B27/0916—Adapting the beam shape of a semiconductor light source such as a laser diode or an LED, e.g. for efficiently coupling into optical fibers
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/09—Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
- G02B27/0938—Using specific optical elements
- G02B27/095—Refractive optical elements
- G02B27/0955—Lenses
- G02B27/0961—Lens arrays
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B21/00—Projectors or projection-type viewers; Accessories therefor
- G03B21/14—Details
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- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B21/00—Projectors or projection-type viewers; Accessories therefor
- G03B21/14—Details
- G03B21/20—Lamp housings
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- F—MECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
- F21—LIGHTING
- F21V—FUNCTIONAL FEATURES OR DETAILS OF LIGHTING DEVICES OR SYSTEMS THEREOF; STRUCTURAL COMBINATIONS OF LIGHTING DEVICES WITH OTHER ARTICLES, NOT OTHERWISE PROVIDED FOR
- F21V13/00—Producing particular characteristics or distribution of the light emitted by means of a combination of elements specified in two or more of main groups F21V1/00 - F21V11/00
Definitions
- the present invention relates to the field of optics, and more particularly to a light source system and a projection apparatus for a laser light source.
- the homogenizing device for the laser light source mainly has a square rod and a compound eye.
- the square bar is divided into a solid square bar and a hollow square bar.
- the principle is to use the light to totally or internally reflect the inside of the square bar to homogenize.
- the number of reflections of the light in the square bar determines the final spot uniformity.
- the length of the rod is longer to ensure the number of reflections, increasing the optical path and volume of the optical system.
- the use of a double compound eye, a double row microlens array, as a light homogenizing device can reduce the volume of the system.
- the Gaussian distribution laser light is incident on the surface of the first row of lens arrays, and is divided into a plurality of small spot units whose size h is the same as the outer shape of the microlens.
- the thickness l is the focal length f of the microlens unit. Therefore, the spot on the surface of the first row of compound eyes is on the focal plane of the second row of compound eyes, and each spot unit on the first row of compound eyes passes through the second row.
- the image is formed by the relay system. Let the focal length of the relay system be f', and the image height on the image plane be h'.
- the image height h' is usually required to be small due to the limitation of the amount of expansion of the entire optical system.
- the diameter of a single laser beam incident on the surface of the compound eye is between 1 mm and 3.5 mm, and it is necessary to ensure that the number of splitting units of the first row of the plurality of laser beams is 15 or more, thereby avoiding serious diffraction effects, and thus the microlens.
- the size of the outer shape is large.
- the double compound eyes need to be thicker to achieve a larger f.
- the requirement of compound eye thickness will bring certain difficulties to the processing of compound eyes. Since the power of the laser is large and the energy is concentrated, the compound eye homogenizing device used must use quartz glass material, and the ordinary plastic material is easily damaged under the irradiation of the laser.
- the process for making quartz glass compound eyes includes lithography processing, mechanical processing, laser processing, bonding, and the like. However, the use of the above process to make quartz glass compound eyes is extremely expensive, and ordinary machining cannot meet the accuracy requirements.
- the technical problem to be solved by the present invention is to provide a light source system and a projection device, which are not only low in cost, high in efficiency, but also uniform in illumination and have a good user experience.
- a technical solution adopted by the present invention is to provide a light source system, the light source system comprising:
- a light source for emitting source light, the source light comprising a plurality of beams parallel to each other;
- the source light is incident on a light homogenizing device for adjusting uniformity of source light
- the light homogenizing device is a double row microlens array, and a lens surface of the double row microlens array
- the center has a recessed area, the plurality of beams avoiding the recessed area on the double-row microlens array;
- a relay module for concentrating and imaging the light beam.
- the distance between the two beams of the plurality of beams of the source light is greater than the maximum diameter of the recessed region.
- the light source system further comprises a compression system on the optical path between the light source and the light homogenizing device for reducing the diameter of the source light.
- the compression system uniformly reduces the distance between the beams.
- the compression system includes at least one positive lens adjacent to the light source and at least one negative lens adjacent to the light homogenizing device, the positive lens for concentrating each of the light beams, and the negative lens for collimating each The light beam.
- the compression system is adapted to change the optical path of the peripheral beam of the source light such that the distance between the peripheral beam of the source and the inner beam of the source is reduced in a first direction perpendicular to the central axis of the source.
- the compression system is further configured to change the optical path of the peripheral beam of the source light such that the distance between the peripheral beam of the source and the inner beam of the source is reduced in a second direction perpendicular to the central axis of the source.
- the compression system includes two sets of first reflecting means disposed opposite each other in a first direction on both sides of the central axis of the source light, and the source light is reduced by the reflection of the first reflecting means to reduce the source light in the first The diameter in one direction.
- the compression system includes two sets of second reflecting devices disposed opposite to each other in a second direction on both sides of the central axis of the source light, and the source light is reduced by the reflection of the second reflecting device to reduce the source light.
- the distance between the two beams of the plurality of beams of the source light is smaller than the maximum diameter of the recessed region.
- the light source system further includes an expansion system on an optical path between the light source and the light homogenizing device for changing an optical path of the inner circumference beam of the source light such that the inner circumference beam of the source light passes through
- the expansion system expands toward the peripheral beam of the light source, avoiding the recessed regions of the light homogenizing device.
- the recessed area has a diameter of 2 mm to 4 mm.
- the light homogenizing device is processed by a sol-gel process.
- another technical solution adopted by the present invention is to provide a projection apparatus including the light source system of any of the foregoing.
- the invention has the beneficial effects that the present invention provides a light source system and a projection device.
- the light source system comprises: a light source, a light homogenizing device and a relay module, wherein the light source is used for emission and is parallel to each other.
- the source light of the plurality of beams, the homogenizing device is a double-row microlens array, the lens surface center of the double-row microlens array has a recessed area, and the plurality of beams avoid the double-row microlens array
- the recessed area solves the technical problem of uneven illumination of the spot deformation in the prior art. Not only low cost, high efficiency, but also uniform illumination, good User experience.
- FIG. 1 is a schematic diagram of a uniform light of a double compound eye in the prior art
- FIG. 2 is a schematic structural view of a first embodiment of a light source system of the present invention
- Figure 3 is a schematic view of the light spot of the structure shown in Figure 2 on the light homogenizing device;
- FIG. 4 is a schematic structural view of a second embodiment of a light source system of the present invention.
- Figure 5 is a schematic view of the light spot of the structure shown in Figure 4 on the light homogenizing device
- FIG. 6 is a schematic structural view of a third embodiment of a light source system of the present invention.
- FIG. 7 is a schematic view of an optical path in a third embodiment of the light source system of the present invention.
- Figure 8 is a schematic illustration of the spot of the structure of Figure 6 on a light homogenizing device.
- FIG. 2 is a schematic structural diagram of a light source system according to a first embodiment of the present invention.
- the light source system of this embodiment includes a light source 401, a compression system 402, a light homogenizing device 403, a relay module 404, and an image plane 405.
- the light source 401 is used to emit source light, wherein the source light comprises a plurality of light beams parallel to each other.
- the light source of this embodiment is a laser light source that emits a plurality of laser beams.
- the image plane 405 is coated with a phosphor, and the laser source light from the light source is imaged at the image plane 405 by the light source system of the present invention.
- the phosphor is excited to emit light.
- the center of the light homogenizing device 403 has a recessed area having a diameter of 2 mm to 4 mm, and a plurality of light beams avoid the recessed area. In the present embodiment, the distance between the two beams of the plurality of beams of the source light is greater than the maximum diameter of the recessed region.
- the relay module 404 is a collecting lens, specifically a convex lens in the present embodiment, for collecting light onto the image plane 405 for imaging.
- a plurality of lenses that function as a converging function may be implemented as long as they can function as a converging light to image plane imaging.
- the compression system 402 is located on the optical path of the laser beam to reduce the diameter of the source light, reduce the distance between different laser beams, and also reduce the length of the system.
- the light homogenizing device 403 is used to adjust the uniformity of the light beam.
- the light homogenizing device 403 is a double-row microlens array whose surface is composed of a plurality of matrix-arranged microlens units.
- the focal length of each lens unit is the same
- the second row array is on the focal plane of the first row of lenses
- the second row array is identical to the first row array and the lens units are in one-to-one correspondence.
- the shape of the microlens is rectangular or hexagonal.
- the laser beam When the respective beams of the source light are incident on the light homogenizing device 403, first, when the laser beam is incident on the first row of arrays, it is divided into a plurality of small regions, and the uniformity of the spot is good in each small region, and the second row array is better.
- the spots of each region in the first row of arrays are superimposed and imaged by subsequent optical systems, and the uniformity of imaging is the superposition and complementarity of the uniformity of each region of the first row, so that better uniformity can be obtained.
- the double-row microlens array is made by a sol-gel process, in particular, quartz glass powder is used as a solute dissolved in a solvent and injected into a mold. Hydrolysis is carried out under the action of a catalyst, a condensation reaction takes place, and a stable transparent sol system is formed. The sol is further aged to form a gel, and the gel is dried and dehydrated to finally form a microlens array assembly.
- the double-row microlens array prepared by the method has low cost and high efficiency, but shrinkage occurs on the surface of the central area, and a certain depression is formed, and FIG. 3 is specifically referred to.
- the source light is first compressed by the compression system 402
- the source light diameter is greatly reduced, about 1.5 mm, and the distance between the light beams is reduced to about 3 mm, and the system length is reduced, so that The recessed area in the center of the double compound eye can be avoided.
- the compression system of the present invention uniformly reduces the distance between the beams, and the laser beam is effectively compressed to avoid the central shrinkage region after being compressed by the compression system 402, thereby avoiding the uneven illumination and affecting the use. effect. Due to the sol-gel method, the cost of the product is also greatly reduced, and the production efficiency is improved.
- the compression system 402 includes a positive lens and a negative lens, wherein the main optical axes of the positive lens and the negative lens are disposed in a coincident manner, and the positive lens and the negative lens are adjacent to the side of the light homogenizing device.
- the focus is coincident, and the positive lens is located in front of the main optical axis, that is, the positive lens is disposed adjacent to the compression system 402, the negative lens is disposed adjacent to the light homogenizing device 403, and the positive lens and the negative lens are adjacent to the side of the light homogenizing device The focus is coincident.
- the positive lens is a convex lens for concentrating each of the light beams
- the negative lens is a concave lens for collimating each of the light beams.
- the present embodiment is substantially the same as the previous embodiment, and the light source system includes a light source 601, a compression system 602, a light homogenizing device 603, a relay module 604, and an image plane 605.
- the light source system includes a light source 601, a compression system 602, a light homogenizing device 603, a relay module 604, and an image plane 605.
- the structure of the compression system 602 is different. Since the source light is composed of a plurality of beams parallel to each other, it has an inner circumference light beam near the center of the light source and a peripheral light beam away from the center of the light source. As shown in FIG. 4, the direction of the vertical source light beam includes a first direction parallel to the plane of view of FIG. 4 and a second direction perpendicular to the plane of view of FIG. In this embodiment, the compression system changes the optical path of the peripheral beam of the source light to reduce the distance between the peripheral beam and the inner beam in a first direction perpendicular to the central axis of the source.
- the compression system 602 includes two sets of first reflecting devices disposed opposite to each other in a first direction on both sides of the central axis of the source light, and the two sets of first reflecting devices respectively compress the light beam in the first direction toward the main optical axis, so that The direction of the beam after compression system 602 is unchanged, but the distance between the peripheral beam and the inner beam is reduced, making it possible to avoid the central constriction of the homogenizing device 603.
- each set of first reflecting means comprises two parallel and oppositely disposed mirrors. After the beam is reflected twice, the direction of the optical path does not change, but is concentrated toward the main optical axis of the source light. At this time, the spot formed on the light homogenizing device 603 is as shown in FIG. 5, effectively avoiding the center shrunken area.
- more than two mirrors may be provided, which can be implemented as long as the above functions can be achieved.
- the light source system includes a light source 801, a compression system 802, a light homogenizing device 803, a relay module 804, and an image plane 805.
- the compression system further includes two sets of second reflecting means disposed opposite to each other in the second direction on both sides of the source light central axis near the light homogenizing device for performing secondary compression on the light beam.
- the second reflecting device is similar in structure to the first reflecting device, and may be a mirror or two or more mirrors, which can be implemented as long as the above functions can be realized.
- a first mirror and a second mirror constituting the first reflecting means and a third mirror and a fourth mirror constituting the second reflecting means are included.
- the beam is sequentially reflected by the first mirror, the second mirror, the third mirror, and the fourth mirror.
- the Y axis is used as the main optical axis of the source light.
- the first mirror and the second mirror are perpendicular to the XY plane
- the third mirror and the fourth mirror are perpendicular to the YZ plane.
- the four-sided mirrors are all at a 45 degree angle to the incident light but are not limited to a 45 degree angle setting.
- the first mirror and the second mirror reduce the distance of the beam from the optical axis in the X direction
- the third mirror and the fourth mirror reduce the distance of the beam from the optical axis in the Z direction.
- the spot formed by it is shown in Fig. 8, so that the light beam further avoids the central shrinkage zone of the light homogenizing device 803 to ensure the reliability of the product.
- This embodiment is substantially the same as the above-described embodiment, except that in the present embodiment, the distance between the two beams of the plurality of beams of the source light is smaller than the maximum diameter of the recessed region.
- an extension system is also provided in the present embodiment.
- the expansion system is located on the optical path between the light source and the light homogenizing device for changing the optical path of the inner wall of the light source, thereby reducing the distance between the peripheral beam and the inner beam, so that the inner beam passes through the extended system
- the peripheral beam direction is extended such that the inner circumference beam is close to the peripheral light and the diameter of the light source does not change, thus avoiding the recessed area at the center of the homogenizing device.
- Embodiments of the present invention also provide a projection apparatus including a light source system as described above.
- the projection device is an educational projector, a laser TV, a micro-projection or a cinema machine.
- the light source system and the projection device of the present invention are not only low in cost, high in efficiency, but also uniform in illumination, and have a good user experience.
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Abstract
A light source system, comprising a light source (401), used for emitting multiple mutually parallel light beams; a light homogenising device (403), used for adjusting the uniformity of the light source, the light homogenising device (403) being a double row micro-lens array, and the source light avoiding a recessed area on the double row micro-lens array; and a relay module (404), used for converging the beam and imaging. Also provided is a projection device.
Description
本发明涉及光学领域,尤其是涉及一种用于激光光源的光源系统和投影设备。The present invention relates to the field of optics, and more particularly to a light source system and a projection apparatus for a laser light source.
目前,用于激光光源的匀光器件主要有方棒和复眼。方棒分为实心方棒和空心方棒,其原理是利用光线在方棒内部全反射或镜面反射进行匀光,由于光线在方棒中的反射次数决定了最终的光斑均匀性,因此,方棒的长度较长以保证反射次数,增加了光学系统的光程与体积。相比之下,利用双复眼,即双排微透镜阵列作为匀光器件可以减小系统的体积。At present, the homogenizing device for the laser light source mainly has a square rod and a compound eye. The square bar is divided into a solid square bar and a hollow square bar. The principle is to use the light to totally or internally reflect the inside of the square bar to homogenize. The number of reflections of the light in the square bar determines the final spot uniformity. The length of the rod is longer to ensure the number of reflections, increasing the optical path and volume of the optical system. In contrast, the use of a double compound eye, a double row microlens array, as a light homogenizing device can reduce the volume of the system.
根据双复眼的匀光原理,如图1所示,高斯分布的激光入射第一排透镜阵列表面,被分割成若干个小的光斑单元,其光斑的尺寸h与微透镜的外形尺寸相同。在双复眼中,其厚度l即为微透镜单元的焦距f,因此,第一排复眼表面的光斑处于第二排复眼的焦平面上,第一排复眼上的每个光斑单元经第二排复眼叠加后经中继系统像成于像平面。设中继系统焦距为f’,像平面上像高为h’,根据成像关系有:对于投影系统而言,由于整个光学系统的扩展量的限制,通常要求像高h’较小。
另外,入射复眼表面的单束激光光束直径在1mm~3.5mm之间,要保证每束激光光束被第一排复眼分割单元的个数在15以上,以此避免严重的衍射效应,因此微透镜的外形尺寸较大。最终需要双复眼比较厚以达到较大的f。According to the uniform light principle of the double compound eyes, as shown in FIG. 1, the Gaussian distribution laser light is incident on the surface of the first row of lens arrays, and is divided into a plurality of small spot units whose size h is the same as the outer shape of the microlens. In the double compound eye, the thickness l is the focal length f of the microlens unit. Therefore, the spot on the surface of the first row of compound eyes is on the focal plane of the second row of compound eyes, and each spot unit on the first row of compound eyes passes through the second row. After the compound eye is superimposed, the image is formed by the relay system. Let the focal length of the relay system be f', and the image height on the image plane be h'. According to the imaging relationship, there are: For projection systems, the image height h' is usually required to be small due to the limitation of the amount of expansion of the entire optical system. In addition, the diameter of a single laser beam incident on the surface of the compound eye is between 1 mm and 3.5 mm, and it is necessary to ensure that the number of splitting units of the first row of the plurality of laser beams is 15 or more, thereby avoiding serious diffraction effects, and thus the microlens. The size of the outer shape is large. Ultimately, the double compound eyes need to be thicker to achieve a larger f.
复眼厚度的要求会给复眼的加工带来一定的难度。由于激光的功率大、能量集中,因此所用的复眼匀光器件必须采用石英玻璃材料,普通的塑料材料在激光的照射下极易损坏。制作石英玻璃复眼的工艺方法有光刻加工、机械加工、激光加工、粘接法等。但是利用上述工艺制作石英玻璃复眼成本极高,而普通的机械加工又不能满足精度的要求。另外还有一种溶胶-凝胶法制作复眼匀光器件的方法,其制作过程中需要一个放大两倍以上的复眼母体,母体通常为塑料材质的复眼,这种方法的成本低、效率高;但若采用此方法制成厚度需求大的双复眼,则制成的石英玻璃双复眼的中心会出现凹陷区域。这种中心有凹陷的复眼会造成成像光斑变形并且照度分布不均匀的现象,因此无法满足用户需求。The requirement of compound eye thickness will bring certain difficulties to the processing of compound eyes. Since the power of the laser is large and the energy is concentrated, the compound eye homogenizing device used must use quartz glass material, and the ordinary plastic material is easily damaged under the irradiation of the laser. The process for making quartz glass compound eyes includes lithography processing, mechanical processing, laser processing, bonding, and the like. However, the use of the above process to make quartz glass compound eyes is extremely expensive, and ordinary machining cannot meet the accuracy requirements. There is also a method for preparing a compound eye homogenizing device by a sol-gel method, which requires a compound eye body which is more than twice as large as the mother eye, and the mother body is usually a compound eye of a plastic material, which is low in cost and high in efficiency; If this method is used to make a double compound eye with a large thickness requirement, a depressed area will appear in the center of the prepared quartz glass double compound eye. Such a compound eye with a concave center causes deformation of the imaging spot and uneven illumination distribution, and thus cannot satisfy the user's needs.
因此,实有必要提供一种新的光源系统及投影设备以解决上述问题。Therefore, it is necessary to provide a new light source system and projection apparatus to solve the above problems.
发明内容Summary of the invention
本发明主要解决的技术问题是提供一种光源系统及投影设备,不仅成本低、效率高,而且照度均匀,具有良好的用户体验。The technical problem to be solved by the present invention is to provide a light source system and a projection device, which are not only low in cost, high in efficiency, but also uniform in illumination and have a good user experience.
为解决上述技术问题,本发明采用的一个技术方案是:提供一种光源系统,所述光源系统包括:
In order to solve the above technical problem, a technical solution adopted by the present invention is to provide a light source system, the light source system comprising:
光源,用于发出源光,所述源光包括相互平行的多束光束;a light source for emitting source light, the source light comprising a plurality of beams parallel to each other;
匀光器件,所述源光入射至匀光器件,所述匀光器件用于调整源光的均匀性,所述匀光器件为双排微透镜阵列,所述双排微透镜阵列的透镜表面中心具有凹陷区,所述多束光束避开所述双排微透镜阵列上的凹陷区;a light homogenizing device, the source light is incident on a light homogenizing device for adjusting uniformity of source light, the light homogenizing device is a double row microlens array, and a lens surface of the double row microlens array The center has a recessed area, the plurality of beams avoiding the recessed area on the double-row microlens array;
中继模组,用于将光束汇聚并成像。A relay module for concentrating and imaging the light beam.
其中,所述源光的多束光束中两两光束之间的距离大于所述凹陷区的最大直径。Wherein, the distance between the two beams of the plurality of beams of the source light is greater than the maximum diameter of the recessed region.
其中,所述光源系统还包括位于所述光源与所述匀光器件之间的光路上用于减小所述源光的直径的压缩系统。其中,所述压缩系统均匀地减小各光束之间的距离。Wherein the light source system further comprises a compression system on the optical path between the light source and the light homogenizing device for reducing the diameter of the source light. Wherein the compression system uniformly reduces the distance between the beams.
其中,所述压缩系统包括靠近所述光源的至少一个正透镜以及靠近所述匀光器件的至少一个负透镜,所述正透镜用于汇聚各所述光束,所述负透镜用于准直各所述光束。Wherein the compression system includes at least one positive lens adjacent to the light source and at least one negative lens adjacent to the light homogenizing device, the positive lens for concentrating each of the light beams, and the negative lens for collimating each The light beam.
其中,所述正透镜和所述负透镜的主光轴重合,且所述正透镜和所述负透镜的靠近所述匀光器件一侧的焦点重合。Wherein the main optical axes of the positive lens and the negative lens coincide, and the focal points of the positive lens and the negative lens adjacent to the side of the light homogenizing device coincide.
其中,所述压缩系统用于改变源光的外围光束的光路,使得在垂直于源光中心轴的第一方向上减少光源的外围光束与光源的内围光束之间的距离。Wherein the compression system is adapted to change the optical path of the peripheral beam of the source light such that the distance between the peripheral beam of the source and the inner beam of the source is reduced in a first direction perpendicular to the central axis of the source.
其中,所述压缩系统还用于改变源光的外围光束的光路,使得在垂直于源光中心轴的第二方向上减少光源的外围光束与光源的内围光束之间的距离。
Wherein, the compression system is further configured to change the optical path of the peripheral beam of the source light such that the distance between the peripheral beam of the source and the inner beam of the source is reduced in a second direction perpendicular to the central axis of the source.
其中,所述压缩系统包括位于源光中心轴两侧沿第一方向相对设置的两组第一反射装置,所述源光经所述第一反射装置的反射作用减小所述源光在第一方向上的直径。Wherein, the compression system includes two sets of first reflecting means disposed opposite each other in a first direction on both sides of the central axis of the source light, and the source light is reduced by the reflection of the first reflecting means to reduce the source light in the first The diameter in one direction.
其中,所述压缩系统包括位于源光中心轴两侧沿第二方向相对设置的两组第二反射装置,所述源光经所述第二反射装置的反射作用减小所述源光在第二方向上的直径。The compression system includes two sets of second reflecting devices disposed opposite to each other in a second direction on both sides of the central axis of the source light, and the source light is reduced by the reflection of the second reflecting device to reduce the source light. The diameter in the two directions.
其中,所述源光的多束光束中两两光束之间的距离小于所述凹陷区的最大直径。Wherein the distance between the two beams of the plurality of beams of the source light is smaller than the maximum diameter of the recessed region.
其中,所述光源系统还包括位于所述光源与所述匀光器件之间的光路上的扩展系统,用于改变源光的内围光束的光路,使得所述源光的内围光束经所述扩展系统向光源的外围光束方向扩展,避开所述匀光器件的凹陷区。Wherein the light source system further includes an expansion system on an optical path between the light source and the light homogenizing device for changing an optical path of the inner circumference beam of the source light such that the inner circumference beam of the source light passes through The expansion system expands toward the peripheral beam of the light source, avoiding the recessed regions of the light homogenizing device.
其中,所述凹陷区的直径为2mm~4mm。Wherein, the recessed area has a diameter of 2 mm to 4 mm.
其中,所述匀光器件由溶胶-凝胶的工艺制程。Wherein, the light homogenizing device is processed by a sol-gel process.
为解决上述技术问题,本发明采用的另一个技术方案是:提供一种投影设备,该投影设备包括前文所述的任一项的光源系统。In order to solve the above technical problem, another technical solution adopted by the present invention is to provide a projection apparatus including the light source system of any of the foregoing.
本发明的有益效果是:区别于现有技术的情况,本发明提供一种光源系统及投影设备,光源系统包括:光源,匀光器件,中继模组,其中,光源用于发射具有相互平行的多束光束的源光,述匀光器件为双排微透镜阵列,所述双排微透镜阵列的透镜表面中心具有凹陷区,所述多束光束避开所述双排微透镜阵列上的凹陷区,解决了现有技术中光斑变形照明不均匀的技术问题。不仅成本低、效率高,而且照度均匀,具有良好
的用户体验。The invention has the beneficial effects that the present invention provides a light source system and a projection device. The light source system comprises: a light source, a light homogenizing device and a relay module, wherein the light source is used for emission and is parallel to each other. The source light of the plurality of beams, the homogenizing device is a double-row microlens array, the lens surface center of the double-row microlens array has a recessed area, and the plurality of beams avoid the double-row microlens array The recessed area solves the technical problem of uneven illumination of the spot deformation in the prior art. Not only low cost, high efficiency, but also uniform illumination, good
User experience.
图1是现有技术中双复眼的匀光原理图;1 is a schematic diagram of a uniform light of a double compound eye in the prior art;
图2是本发明光源系统的第一种实施方式的结构示意图;2 is a schematic structural view of a first embodiment of a light source system of the present invention;
图3是图2所示结构在匀光器件上的光斑示意图;Figure 3 is a schematic view of the light spot of the structure shown in Figure 2 on the light homogenizing device;
图4是本发明光源系统的第二种实施方式的结构示意图;4 is a schematic structural view of a second embodiment of a light source system of the present invention;
图5是图4所示结构在匀光器件上的光斑示意图;Figure 5 is a schematic view of the light spot of the structure shown in Figure 4 on the light homogenizing device;
图6是本发明光源系统的第三种实施方式的结构示意图;6 is a schematic structural view of a third embodiment of a light source system of the present invention;
图7是本发明光源系统的第三种实施方式中光路示意图;7 is a schematic view of an optical path in a third embodiment of the light source system of the present invention;
图8是图6所示结构在匀光器件上的光斑示意图。Figure 8 is a schematic illustration of the spot of the structure of Figure 6 on a light homogenizing device.
应当理解,此处所描述的具体实施例仅仅用以解释本发明,并不用于限定本发明。It is understood that the specific embodiments described herein are merely illustrative of the invention and are not intended to limit the invention.
实施例一Embodiment 1
请参阅图2,是本发明第一种实施例提供的一种光源系统的结构示意图。如图2所示,本实施例的光源系统包括光源401、压缩系统402、匀光器件403、中继模组404以及像平面405。Please refer to FIG. 2 , which is a schematic structural diagram of a light source system according to a first embodiment of the present invention. As shown in FIG. 2, the light source system of this embodiment includes a light source 401, a compression system 402, a light homogenizing device 403, a relay module 404, and an image plane 405.
其中,光源401用于发出源光,其中源光包括相互平行的多束光束。本实施例的光源为激光光源,发出多束激光光束。像平面405上涂覆有荧光粉,光源发出的激光源光通过本发明光源系统在像平面405成像并
激发荧光粉发光。匀光器件403的中心具有直径为2mm~4mm的凹陷区,多束光束避开该凹陷区。在本实施方式中,源光的多束光束中两两光束之间的距离大于所述凹陷区的最大直径。中继模组404为收集透镜,具体在本实施方式中为一凸透镜,其用于将光线汇聚到像平面405上成像。在可选择的其他实施方式中,也可以为起到汇聚作用的多个透镜,只要能够起到汇聚光线到像平面成像的作用,既是可以实施的。Wherein, the light source 401 is used to emit source light, wherein the source light comprises a plurality of light beams parallel to each other. The light source of this embodiment is a laser light source that emits a plurality of laser beams. The image plane 405 is coated with a phosphor, and the laser source light from the light source is imaged at the image plane 405 by the light source system of the present invention.
The phosphor is excited to emit light. The center of the light homogenizing device 403 has a recessed area having a diameter of 2 mm to 4 mm, and a plurality of light beams avoid the recessed area. In the present embodiment, the distance between the two beams of the plurality of beams of the source light is greater than the maximum diameter of the recessed region. The relay module 404 is a collecting lens, specifically a convex lens in the present embodiment, for collecting light onto the image plane 405 for imaging. In other optional embodiments, a plurality of lenses that function as a converging function may be implemented as long as they can function as a converging light to image plane imaging.
压缩系统402位于激光光束的光路上,用于减小源光的直径,减小不同激光光束之间的距离,同时也可以缩小系统的长度。匀光器件403用于调整光束的均匀性,在本实施方式中,匀光器件403为双排微透镜阵列,其表面由若干矩阵排列的微透镜单元组成。其中,每个透镜单元的焦距相同,第二排阵列处于第一排透镜的焦平面上,并且第二排阵列与第一排阵列完全相同且透镜单元一一对应。具体的,微透镜的外形为矩形或六边形。The compression system 402 is located on the optical path of the laser beam to reduce the diameter of the source light, reduce the distance between different laser beams, and also reduce the length of the system. The light homogenizing device 403 is used to adjust the uniformity of the light beam. In the present embodiment, the light homogenizing device 403 is a double-row microlens array whose surface is composed of a plurality of matrix-arranged microlens units. Wherein, the focal length of each lens unit is the same, the second row array is on the focal plane of the first row of lenses, and the second row array is identical to the first row array and the lens units are in one-to-one correspondence. Specifically, the shape of the microlens is rectangular or hexagonal.
当源光的各个光束射入匀光器件403时,首先,激光光束入射第一排阵列时被分割成很多个小区域,在每个小区域内光斑的均匀性是较好的,第二排阵列将第一排阵列中每个区域的光斑叠加并通过后续的光学系统成像,所成像的均匀性是第一排每个区域均匀性的叠加与互补,因此,可以得到较好的均匀性。When the respective beams of the source light are incident on the light homogenizing device 403, first, when the laser beam is incident on the first row of arrays, it is divided into a plurality of small regions, and the uniformity of the spot is good in each small region, and the second row array is better. The spots of each region in the first row of arrays are superimposed and imaged by subsequent optical systems, and the uniformity of imaging is the superposition and complementarity of the uniformity of each region of the first row, so that better uniformity can be obtained.
其中,双排微透镜阵列为采用溶胶-凝胶法的工艺制成,具体为采用石英玻璃粉作为溶质溶于溶剂中,注入模具中。在催化剂的作用下进行水解,发生缩合反应,并形成稳定的透明溶胶体系。溶胶再经陈化处理后聚合形成凝胶,凝胶经干燥、脱水后最终制备成微透镜阵列组件。这
种方式制备的双排微透镜阵列成本低,效率高,但是在中心区的表面会有缩水现象发生,并形成一定的凹陷,具体参照图3。而在本实施方式中,由于源光先经过压缩系统402压缩,源光直径大大减小,约为1.5mm,光束彼此间距减小,减小到约为3mm,同时系统长度减小,因此恰好可以避开双复眼的中心的凹陷区域。参照图3所示,本发明压缩系统均匀地减小了各光束之间的距离,激光光束经过压缩系统402的压缩后有效地避开了中心缩水的区域,避免了光照的不均匀而影响使用效果。由于采用溶胶-凝胶法,也极大地降低了产品的成本,提高了生产效率。Among them, the double-row microlens array is made by a sol-gel process, in particular, quartz glass powder is used as a solute dissolved in a solvent and injected into a mold. Hydrolysis is carried out under the action of a catalyst, a condensation reaction takes place, and a stable transparent sol system is formed. The sol is further aged to form a gel, and the gel is dried and dehydrated to finally form a microlens array assembly. This
The double-row microlens array prepared by the method has low cost and high efficiency, but shrinkage occurs on the surface of the central area, and a certain depression is formed, and FIG. 3 is specifically referred to. In the present embodiment, since the source light is first compressed by the compression system 402, the source light diameter is greatly reduced, about 1.5 mm, and the distance between the light beams is reduced to about 3 mm, and the system length is reduced, so that The recessed area in the center of the double compound eye can be avoided. Referring to FIG. 3, the compression system of the present invention uniformly reduces the distance between the beams, and the laser beam is effectively compressed to avoid the central shrinkage region after being compressed by the compression system 402, thereby avoiding the uneven illumination and affecting the use. effect. Due to the sol-gel method, the cost of the product is also greatly reduced, and the production efficiency is improved.
具体在本实施方式中,压缩系统402包括正透镜和负透镜,其中,正透镜和负透镜的主光轴重合设置,且所述正透镜和所述负透镜的靠近所述匀光器件一侧的焦点重合,且正透镜位于主光轴前方,即正透镜靠近压缩系统402设置,负透镜靠近匀光器件403设置,且所述正透镜和所述负透镜的靠近所述匀光器件一侧的焦点重合。其中,正透镜为凸透镜用于汇聚各所述光束,负透镜为凹透镜,用于准直各所述光束。相互平行的激光光束进入压缩系统402后,首先经过正透镜汇聚,再经过负透镜后使得出射光路平行于入射光路射出。这样,经过压缩系统402后的光束的方向不变,但光束之间的距离缩小,使得光束能够避开匀光器件403的中心缩水区。上述仅为最优的实施方式,实施上,压缩系统402也可以为多个凸透镜和多个凹透镜的组合,只要能够实现上述功能,即是可以实施的。Specifically, in the present embodiment, the compression system 402 includes a positive lens and a negative lens, wherein the main optical axes of the positive lens and the negative lens are disposed in a coincident manner, and the positive lens and the negative lens are adjacent to the side of the light homogenizing device. The focus is coincident, and the positive lens is located in front of the main optical axis, that is, the positive lens is disposed adjacent to the compression system 402, the negative lens is disposed adjacent to the light homogenizing device 403, and the positive lens and the negative lens are adjacent to the side of the light homogenizing device The focus is coincident. Wherein, the positive lens is a convex lens for concentrating each of the light beams, and the negative lens is a concave lens for collimating each of the light beams. After the mutually parallel laser beams enter the compression system 402, they are first concentrated by a positive lens, and then passed through a negative lens to cause the outgoing light path to be emitted parallel to the incident optical path. Thus, the direction of the beam after passing through the compression system 402 is unchanged, but the distance between the beams is reduced, so that the beam can avoid the central constriction of the homogenizing device 403. The above is only an optimal embodiment. In practice, the compression system 402 may also be a combination of a plurality of convex lenses and a plurality of concave lenses, and can be implemented as long as the above functions can be realized.
实施例二
Embodiment 2
参照图4和图5所示,本实施方式与上一种实施方式大致相同,光源系统包括光源601、压缩系统602、匀光器件603、中继模组604以及像平面605。4 and 5, the present embodiment is substantially the same as the previous embodiment, and the light source system includes a light source 601, a compression system 602, a light homogenizing device 603, a relay module 604, and an image plane 605.
区别在于,压缩系统602的结构不同。由于源光为相互平行的多束光束组成,因此具有靠近光源中心的内围光束和远离光源中心的外围光束。如图4所示,其中垂直源光光束的方向包括平行于图4视平面的第一方向和垂直于图4视平面的第二方向。本实施方式中,压缩系统改变了源光的外围光束的光路在垂直于源光中心轴的第一方向上减少了外围光束与内围光束之间的距离。具体的,压缩系统602包括位于源光中心轴两侧沿第一方向相对设置的两组第一反射装置,两组第一反射装置分别将光束沿第一方向向主光轴方向压缩,使得经过压缩系统602后光束的方向不变,但外围光束与内围光束之间的距离缩小,使得能够避开匀光器件603的中心缩水区。The difference is that the structure of the compression system 602 is different. Since the source light is composed of a plurality of beams parallel to each other, it has an inner circumference light beam near the center of the light source and a peripheral light beam away from the center of the light source. As shown in FIG. 4, the direction of the vertical source light beam includes a first direction parallel to the plane of view of FIG. 4 and a second direction perpendicular to the plane of view of FIG. In this embodiment, the compression system changes the optical path of the peripheral beam of the source light to reduce the distance between the peripheral beam and the inner beam in a first direction perpendicular to the central axis of the source. Specifically, the compression system 602 includes two sets of first reflecting devices disposed opposite to each other in a first direction on both sides of the central axis of the source light, and the two sets of first reflecting devices respectively compress the light beam in the first direction toward the main optical axis, so that The direction of the beam after compression system 602 is unchanged, but the distance between the peripheral beam and the inner beam is reduced, making it possible to avoid the central constriction of the homogenizing device 603.
具体的,在本实施方式中,每组第一反射装置包括两个平行且相对设置的反射镜。光束经过二次反射后,光路的方向不变,而向源光主光轴方向聚拢。此时在匀光器件603上形成的光斑如图5所示,有效地避开了中心缩水区。当然,在可选择的其他实施方式中,也可以设置两个以上的反射镜,只要能够实现上述功能,即是可以实施的。Specifically, in the present embodiment, each set of first reflecting means comprises two parallel and oppositely disposed mirrors. After the beam is reflected twice, the direction of the optical path does not change, but is concentrated toward the main optical axis of the source light. At this time, the spot formed on the light homogenizing device 603 is as shown in FIG. 5, effectively avoiding the center shrunken area. Of course, in other alternative embodiments, more than two mirrors may be provided, which can be implemented as long as the above functions can be achieved.
实施例三Embodiment 3
参照图6和图7所示,本实施方式是在上述两种实施例的基础上做了进一步的改进。参照图6和图7,以在第二种实施例的基础上改进为
例进行说明,事实上,也可以在第一种实施例的基础上进行改进。Referring to Figures 6 and 7, the present embodiment is further improved on the basis of the above two embodiments. Referring to Figures 6 and 7, improved on the basis of the second embodiment
The example is explained, in fact, it is also possible to improve on the basis of the first embodiment.
光源系统包括光源801、压缩系统802、匀光器件803、中继模组804以及像平面805。The light source system includes a light source 801, a compression system 802, a light homogenizing device 803, a relay module 804, and an image plane 805.
在上述实施例的基础上,进一步的,压缩系统还包括靠近匀光器件的位于源光中心轴两侧沿第二方向相对设置的两组第二反射装置,用于对光束进行二次压缩,改变所述的外围光束的光路,使得在第二方向上减小了光源的外围光束与内围光束之间的距离,源光经所述第二反射装置的反射作用减小在第二方向上的直径。其中第二反射装置与第一反射装置的结构类似,可以为反射镜,也可以设置两个或两个以上的反射镜,只要能够实现上述功能,即是可以实施的。具体在本实施方式中,包括组成第一反射装置的第一反射镜、和第二反射镜以及组成第二反射装置的第三反射镜和第四反射镜。参照图7所示,以其中一束光束的路径为例,光束顺序经第一反射镜、第二反射镜、第三反射镜和第四反射镜反射。其中Y轴做为源光的主光轴。其中第一反射镜和第二反射镜垂直于XY平面,第三反射镜和第四反射镜垂直于YZ平面。四面反射镜都与入射光呈45度角但不限于45度角设置。第一反射镜和第二反射镜使得光束与光轴在X方向上的距离减小,第三反射镜和第四反射镜使得光束与光轴在Z方向上的距离减小。从而使得周围的光束往光轴靠近。其形成的光斑参照图8所示,使得光束进一步避开匀光器件803的中心缩水区,以保证产品的可靠性。On the basis of the above embodiments, further, the compression system further includes two sets of second reflecting means disposed opposite to each other in the second direction on both sides of the source light central axis near the light homogenizing device for performing secondary compression on the light beam. Changing the optical path of the peripheral beam such that the distance between the peripheral beam and the inner beam of the light source is reduced in the second direction, and the source light is reduced in the second direction by the reflection of the second reflecting means diameter of. The second reflecting device is similar in structure to the first reflecting device, and may be a mirror or two or more mirrors, which can be implemented as long as the above functions can be realized. Specifically, in the present embodiment, a first mirror and a second mirror constituting the first reflecting means and a third mirror and a fourth mirror constituting the second reflecting means are included. Referring to FIG. 7, taking the path of one of the beams as an example, the beam is sequentially reflected by the first mirror, the second mirror, the third mirror, and the fourth mirror. The Y axis is used as the main optical axis of the source light. Wherein the first mirror and the second mirror are perpendicular to the XY plane, and the third mirror and the fourth mirror are perpendicular to the YZ plane. The four-sided mirrors are all at a 45 degree angle to the incident light but are not limited to a 45 degree angle setting. The first mirror and the second mirror reduce the distance of the beam from the optical axis in the X direction, and the third mirror and the fourth mirror reduce the distance of the beam from the optical axis in the Z direction. Thereby the surrounding beams are brought closer to the optical axis. The spot formed by it is shown in Fig. 8, so that the light beam further avoids the central shrinkage zone of the light homogenizing device 803 to ensure the reliability of the product.
实施例四
Embodiment 4
本实施方式与前述的实施方式大致相同,区别在于,在本实施方式中,源光的多束光束中两两光束之间的距离小于所述凹陷区的最大直径。与之相应的,本实施方式中还设置扩展系统。This embodiment is substantially the same as the above-described embodiment, except that in the present embodiment, the distance between the two beams of the plurality of beams of the source light is smaller than the maximum diameter of the recessed region. Correspondingly, an extension system is also provided in the present embodiment.
扩展系统位于所述光源与所述匀光器件之间的光路上用于改变光源的内围光束的光路,从而缩小外围光束与内围光束之间的距离,使得内围光束经过扩展系统后向外围光束方向扩展,使得内围光束靠近外围光而光源的直径不改变,这样就避开了匀光器件中心的凹陷区。The expansion system is located on the optical path between the light source and the light homogenizing device for changing the optical path of the inner wall of the light source, thereby reducing the distance between the peripheral beam and the inner beam, so that the inner beam passes through the extended system The peripheral beam direction is extended such that the inner circumference beam is close to the peripheral light and the diameter of the light source does not change, thus avoiding the recessed area at the center of the homogenizing device.
本发明实施例还提供一种投影设备,该投影设备包括如前文所述的光源系统。投影设备为教育投影仪、激光电视、微投或影院机。Embodiments of the present invention also provide a projection apparatus including a light source system as described above. The projection device is an educational projector, a laser TV, a micro-projection or a cinema machine.
综上所述,本发明的光源系统及投影设备,不仅成本低、效率高,而且照度均匀,具有良好的用户体验。In summary, the light source system and the projection device of the present invention are not only low in cost, high in efficiency, but also uniform in illumination, and have a good user experience.
以上所述仅为本发明的实施例,并非因此限制本发明的专利范围,凡是利用本发明说明书及附图内容所作的等效结构或等效流程变换,或直接或间接运用在其他相关的技术领域,均同理包括在本发明的专利保护范围内。
The above is only the embodiment of the present invention, and is not intended to limit the scope of the invention, and the equivalent structure or equivalent process transformation of the present invention and the contents of the drawings may be directly or indirectly applied to other related technologies. The fields are all included in the scope of patent protection of the present invention.
Claims (15)
- 一种光源系统,其特征在于,所述光源系统包括:A light source system, characterized in that the light source system comprises:光源,用于发出源光,所述源光包括相互平行的多束光束;a light source for emitting source light, the source light comprising a plurality of beams parallel to each other;匀光器件,所述源光入射至匀光器件,所述匀光器件用于调整所述源光的均匀性,所述匀光器件为双排微透镜阵列,所述双排微透镜阵列的透镜表面中心具有凹陷区,所述多束光束避开所述双排微透镜阵列上的凹陷区;a light homogenizing device, the source light is incident on a light homogenizing device for adjusting uniformity of the source light, the light homogenizing device is a double row microlens array, and the double row microlens array The center of the lens surface has a recessed area, the plurality of beams avoiding the recessed area on the double-row microlens array;中继模组,用于将光束汇聚并成像。A relay module for concentrating and imaging the light beam.
- 根据权利要求1所述的光源系统,其特征在于,所述源光的多束光束中两两光束之间的距离大于所述凹陷区的最大直径。The light source system according to claim 1, wherein a distance between two of the plurality of beams of the source light is greater than a maximum diameter of the recessed region.
- 根据权利要求2所述的光源系统,其特征在于,所述光源系统还包括位于所述光源与所述匀光器件之间的光路上用于减小所述源光的直径的压缩系统。The light source system of claim 2 wherein said light source system further comprises a compression system for reducing the diameter of said source light on an optical path between said light source and said light homogenizing means.
- 根据权利要求3所述的光源系统,其特征在于,所述压缩系统均匀地减小各光束之间的距离。The light source system of claim 3 wherein said compression system uniformly reduces the distance between the beams.
- 根据权利要求4所述的光源系统,其特征在于,所述压缩系统包括靠近所述光源的至少一个正透镜以及靠近所述匀光器件的至少一个负透镜,所述正透镜用于汇聚各所述光束,所述负透镜用于准直各所述光束。A light source system according to claim 4, wherein said compression system includes at least one positive lens adjacent said light source and at least one negative lens adjacent said light homogenizing means for concentrating each The light beam is used to collimate each of the light beams.
- 根据权利要求5所述的光源系统,其特征在于,所述正透镜与所述负透镜的主光轴重合,且所述正透镜和所述负透镜的靠近所述匀光 器件一侧的焦点重合。The light source system according to claim 5, wherein said positive lens coincides with a main optical axis of said negative lens, and said positive lens and said negative lens are close to said uniform light The focus on one side of the device coincides.
- 根据权利要求3所述的光源系统,其特征在于,所述压缩系统用于改变所述源光的外围光束的光路,使得在垂直于源光中心轴的第一方向上减少所述光源的外围光束与所述光源的内围光束之间的距离。The light source system according to claim 3, wherein said compression system is adapted to change an optical path of a peripheral beam of said source light such that a periphery of said light source is reduced in a first direction perpendicular to a central axis of said source light The distance between the beam and the inner beam of the source.
- 根据权利要求7所述的光源系统,其特征在于,所述压缩系统还用于改变所述源光的外围光束的光路,使得在垂直于源光中心轴的第二方向上减少所述光源的外围光束与所述光源的内围光束之间的距离。The light source system according to claim 7, wherein said compression system is further configured to change an optical path of a peripheral beam of said source light such that said source is reduced in a second direction perpendicular to a central axis of said source light The distance between the peripheral beam and the inner beam of the source.
- 根据权利要求7所述的光源系统,其特征在于,所述压缩系统包括位于源光中心轴两侧沿第一方向相对设置的两组第一反射装置,所述源光经所述第一反射装置的反射作用减小在第一方向上的直径。The light source system according to claim 7, wherein said compression system comprises two sets of first reflecting means disposed opposite each other in a first direction on both sides of a source light central axis, said source light passing said first reflection The reflection of the device reduces the diameter in the first direction.
- 根据权利要求9所述的光源系统,其特征在于,所述压缩系统还包括位于源光中心轴两侧沿第二方向相对设置的两组第二反射装置,所述源光经所述第二反射装置的反射作用减小在第二方向上的直径。The light source system according to claim 9, wherein the compression system further comprises two sets of second reflecting means disposed opposite each other in a second direction on both sides of the central axis of the source light, the source light passing through the second The reflection of the reflecting means reduces the diameter in the second direction.
- 根据权利要求1所述的光源系统,其特征在于,所述源光的多束光束中两两光束之间的距离小于所述凹陷区的最大直径。The light source system according to claim 1, wherein a distance between two of the plurality of beams of the source light is smaller than a maximum diameter of the recessed region.
- 根据权利要求11所述的光源系统,其特征在于,所述光源系统还包括位于所述光源与所述匀光器件之间的光路上的扩展系统,用于改变所述源光的内围光束的光路,使得所述源光的内围光束向所述光源的外围光束方向扩展,从而避开所述匀光器件的凹陷区。The light source system according to claim 11, wherein said light source system further comprises an expansion system on an optical path between said light source and said light homogenizing means for changing an inner peripheral beam of said source light The light path is such that the inner peripheral light beam of the source light expands toward the peripheral beam of the light source, thereby avoiding the recessed region of the light homogenizing device.
- 根据权利要求1所述的光源系统,其特征在于,所述凹陷区的直径为2mm~4mm。The light source system according to claim 1, wherein the recessed portion has a diameter of 2 mm to 4 mm.
- 根据权利要求1所述的光源系统,其特征在于,所述匀光器件 由溶胶-凝胶的工艺制程。The light source system of claim 1 wherein said light homogenizing device Process by sol-gel process.
- 一种投影设备,其特征在于,所述投影设备包括如权利要求1-14任一项所述的光源系统。 A projection apparatus, characterized in that the projection apparatus comprises the light source system according to any one of claims 1-14.
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CN103969933A (en) * | 2013-02-04 | 2014-08-06 | 深圳市光峰光电技术有限公司 | Laser light source, wavelength conversion light source, integrating light source and projection display device |
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